2017
DOI: 10.1098/rsos.160698
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Nonlinear amplitude dynamics in flagellar beating

Abstract: The physical basis of flagellar and ciliary beating is a major problem in biology which is still far from completely understood. The fundamental cytoskeleton structure of cilia and flagella is the axoneme, a cylindrical array of microtubule doublets connected by passive cross-linkers and dynein motor proteins. The complex interplay of these elements leads to the generation of self-organized bending waves. Although many mathematical models have been proposed to understand this process, few attempts have been ma… Show more

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Cited by 50 publications
(135 citation statements)
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References 42 publications
(140 reference statements)
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“…The boundary conditions are non-local due to the accumulative dependence of sliding moments along the bundle, and generally unknown during the dynamics. This is becomes even more challenging when the bundle is driven via the molecular motor activity [20,68], which may explain the reason why numerical investigation of geometrically exact bundle systems are still lacking, for both active and passive cases [68]. The coarse-grained formulation brakes the contribution of the sliding filament moments for each segments simply as…”
Section: Cross-linked Filament Bundles and Flagellamentioning
confidence: 99%
“…The boundary conditions are non-local due to the accumulative dependence of sliding moments along the bundle, and generally unknown during the dynamics. This is becomes even more challenging when the bundle is driven via the molecular motor activity [20,68], which may explain the reason why numerical investigation of geometrically exact bundle systems are still lacking, for both active and passive cases [68]. The coarse-grained formulation brakes the contribution of the sliding filament moments for each segments simply as…”
Section: Cross-linked Filament Bundles and Flagellamentioning
confidence: 99%
“…Furthermore, the standing waves in the z-plane are unlikely to be achieved via molecular motor dynamics alone as this would require a fast, synchronised motor coordination over long flagellar distances, not yet reported in the literature. Indeed, molecular motor self-organisation is manifested through time-delayed oscillations along the flagellum [38,63,64] which leads to the generation of propagating waves, and therefore the most likely mechanism to govern the asymmetric travelling waves observed in the b-plane ( Fig. 8(a)) [1,2,5].…”
Section: Discussionmentioning
confidence: 99%
“…We employed principal component analysis (PCA) on the 3D flagellar shape at the comoving, X c (s, t), and comoving-rolling, X cr (s, t), frames of reference. For this, we generalised the previous PCA of scalar quantities [26,38,65,66] to three-dimensional vectorial functions, in which each spatial coordinate represents an spatiotemporal map in arclength and time, (s, t).…”
Section: Principal Component Analysis Of the 3d Waveformmentioning
confidence: 99%
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“…The potential applications for a fast and accurate filament modeling framework are numerous. There has long been interest in understanding the mechanics and regulation of sperm flagellar movement, in particular problems relating to: understanding the mechanical struc-ture and motor regulation [5,[12][13][14], investigating the response of the flagellar beat to its rheological environment [15][16][17], understanding the dynamics of sperm due to surrounding solid walls [18,19], and studying the effect of viscosity on sperm swimming [20]. For a detailed review surrounding the importance of the sperm flagellum see Gallagher et al [21].…”
Section: Introductionmentioning
confidence: 99%